Electric Potential @ center of an equilateral triangle

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SUMMARY

The electric potential at point P, the center of an equilateral triangle with side length 2a and total charge Q, is calculated as k(Q/a) ln(2 + √3). The solution involves integrating the electric potential contributions from each side of the triangle, utilizing the equation v(r) = kq/r and the integral ∆v = -∫E∙ds. The integration limits are determined by the symmetry of the triangle, allowing for simplification by integrating from 0 to a and multiplying by 3 for the three sides.

PREREQUISITES
  • Understanding of electric potential and electric field concepts
  • Familiarity with calculus, specifically integration techniques
  • Knowledge of the properties of equilateral triangles
  • Proficiency in using the equation v(r) = kq/r for electric potential calculations
NEXT STEPS
  • Study the derivation of electric potential from continuous charge distributions
  • Learn about symmetry in electrostatics and its applications in potential calculations
  • Explore advanced integration techniques relevant to physics problems
  • Investigate the implications of using different reference points for electric potential
USEFUL FOR

This discussion is beneficial for physics students, educators, and anyone involved in electrostatics, particularly those tackling problems related to electric potential in geometrically symmetric charge distributions.

Nyquilt
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Homework Statement



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What is the electric potential at point P, the center of an equilateral triangle with side length of 2a and total charge of Q? Use infinity as the reference point.


Homework Equations



∆v = -∫E∙ds
v(r)= kq/r

The Attempt at a Solution



I already have the answer which is k(Q/a) ln(2+sqrt(3)) but I don't know how to get it. This is what I tried:

v = kq/r = ∫kdq/r = ∫k lamda dx/r = k lamda ∫dx/sqrt(x^2 + (a/sqrt(3))^2) = k lamda ln(x + sqrt(x^2 + (a/sqrt(3))^2)).

I evaluate that integral from 0 to 2a

k lamda ln(2a - sqrt(4a^2 + (a^2)/3) - k lamda ln(a/sqrt(3))
= k lamda ln(2sqrt(3) - sqrt(13)) = kQ/(2a) ln(2sqrt(3) - sqrt(13))
 
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Your substitution for r = sqrt(x^2 + (a/sqrt(3))^2 Fixes the origin for your x-axis somewhere. Where is that point? How does that change the limits for your integral?
 
Hmm I guess the origin for the x-axis is at the axis of symmetry. If that's the case then I integrate from -a to a?
 
Yes. Either that, or you can further exploit symetry by only integrating from 0 to a and multiplying by 2. Also, your integral was the potential from only one side of the triangle. I'm not sure if you multiplied by 3.
 
That worked great. Thanks a lot for the help. I was stuck on this for a while.
 

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